Haze Communication using the CAMNET and IMPROVE Archives: Case Study at Acadia National Park

Similar documents
Big Bend Regional Aerosol & Visibility Observational Study

5. Light Extinction In The Desert Southwest

6.5 Interrelationships of Fine Mass, Sulfur and Absorption Daily Scatter Plots Shenandoah National Park

Who is polluting the Columbia River Gorge?

Review of the IMPROVE Equation for Estimating Ambient Light Extinction

Continuous measurement of airborne particles and gases

Update on IMPROVE Light Extinction Equation and Natural Conditions Estimates. Tom Moore, WRAP Technical Coordinator. May 23, 2006

Figure 1. A terrain map of Texas and Mexico as well as some major cites and points of interest to the BRAVO study.

3) Big Bend s Aerosol and Extinction Budgets during BRAVO

2002 Year in Review Project Manager Gary Kleiman Principal Contributors (NESCAUM) Al Leston John Graham George Allen Gary Kleiman

Aerosol Optical Properties

Regional Haze Metrics Trends and HYSPLIT Trajectory Analyses. May 2017

Resolving Autocorrelation Bias in the Determination of the Extinction Efficiency of Fugitive Dust from Cattle Feedyards

6. Chemical Contributions to Extinction

Spatial and Seasonal Patterns and Temporal Variability of Haze and its Constituents in the United States

Review of the IMPROVE Equation for Reconstructing Extinction from Aerosol Measurements

12. ATTRIBUTION RECONCILIATION, CONCEPTUAL MODEL, AND LESSONS LEARNED

CHAPTER 8. AEROSOLS 8.1 SOURCES AND SINKS OF AEROSOLS

Comparison of Particulate Monitoring Methods at Fort Air Partnership Monitoring Stations

PRELIMINARY DRAFT FOR DISCUSSION PURPOSES

UNCERTAINTY ASSOCIATED WITH ESTIMATING A SHORT-TERM (1 3 HR) PARTICULATE MATTER CONCENTRATION FROM A HUMAN-SIGHTED VISUAL RANGE

DOCUMENT HISTORY. Initials Section/s Modified Brief Description of Modifications

HIPS data are now reported with a consistent calibration (2003 present) what do they say?

Lecture 26. Regional radiative effects due to anthropogenic aerosols. Part 2. Haze and visibility.

Physicochemical and Optical Properties of Aerosols in South Korea

Chapter 2 Available Solar Radiation

John G. Watson Judith C. Chow Mark C. Green Xiaoliang Wang Desert Research Institute, Reno, NV

COUPLING A DISTRIBUTED HYDROLOGICAL MODEL TO REGIONAL CLIMATE MODEL OUTPUT: AN EVALUATION OF EXPERIMENTS FOR THE RHINE BASIN IN EUROPE

Uncertainties in PM2.5 Gravimetric and Speciation Measurements and What Can We Learn from Them

CLIMATE CHANGE Albedo Forcing ALBEDO FORCING

Climatic and Ecological Conditions in the Klamath Basin of Southern Oregon and Northern California: Projections for the Future

Hygroscopic Growth of Aerosols and their Optical Properties

Visibility and Air Quality Measurement Methods Used by the National Park Service

Collection Efficiency: A summary of what we know so far.

Measuring & Monitoring Pn. Light Roberto Lopez, Purdue Univ.

Agricultural Science Climatology Semester 2, Anne Green / Richard Thompson

YACT (Yet Another Climate Tool)? The SPI Explorer

JOURNAL OF INTERNATIONAL ACADEMIC RESEARCH FOR MULTIDISCIPLINARY Impact Factor 1.393, ISSN: , Volume 2, Issue 4, May 2014

Memo. I. Executive Summary. II. ALERT Data Source. III. General System-Wide Reporting Summary. Date: January 26, 2009 To: From: Subject:

Exercise 6. Solar Panel Orientation EXERCISE OBJECTIVE DISCUSSION OUTLINE. Introduction to the importance of solar panel orientation DISCUSSION

Item 1: Edits to Select Appendix S Class I Air Dispersion Modeling Report text

Global Climates. Name Date

Introduction to Open-Path Transmissometry as a Surrogate Measure of Ambient PM at Cattle Feedyards

INSITU project within AeroCom Phase III: Description and Model Output Request

The Importance of Ammonia in Modeling Atmospheric Transport and Deposition of Air Pollution. Organization of Talk:

Local Ctimatotogical Data Summary White Hall, Illinois

Interannual variation of MODIS NDVI in Lake Taihu and its relation to climate in submerged macrophyte region

Prentice Hall EARTH SCIENCE. Tarbuck Lutgens

Can a change of single scattering albedo in Amami-Oshima in a low pressure condition be explained by GCM simulations?

Disentangling Impacts of Climate & Land Use Changes on the Quantity & Quality of River Flows in Southern Ontario

Aerosol type how to use the information from satellites for models???

Dust storm variability over EGYPT By Fathy M ELashmawy Egyptian Meteorological Authority

Bryan Butler. National Radio Astronomy Observatory. November 23, 1998

2008 Growing Season. Niagara Region

What are Aerosols? Suspension of very small solid particles or liquid droplets Radii typically in the range of 10nm to

PROPOSED FLAG LEVEL II AND III VISIBILITY ASSESSMENT

Communicating Climate Change Consequences for Land Use

ATOC 3500/CHEM 3152 Week 9, March 8, 2016

Response to Reviewer s comments

ONE-YEAR EXPERIMENT IN NUMERICAL PREDICTION OF MONTHLY MEAN TEMPERATURE IN THE ATMOSPHERE-OCEAN-CONTINENT SYSTEM

GEO 101, Feb 4, 2014 Finish isolines Atmosphere intro Variation in incoming solar radiation. Freezing rain is supercooled liquid water

Central Ohio Air Quality End of Season Report. 111 Liberty Street, Suite 100 Columbus, OH Mid-Ohio Regional Planning Commission

CLIMATE OVERVIEW. Thunder Bay Climate Overview Page 1 of 5

Will a warmer world change Queensland s rainfall?

Drought Characterization. Examination of Extreme Precipitation Events

Lecture 2: Global Energy Cycle

The Climate of Payne County

2.444 A FEASIBILTY STUDY OF THE MARGA TOOL AS AN AEROSOL ANALYZER

The Climate of Kiowa County

Variability of Reference Evapotranspiration Across Nebraska

7. Aerosols and Climate

The Climate of Murray County

CHAPTER 7 AEROSOL ACIDITY

- global radiative energy balance

Chiang Rai Province CC Threat overview AAS1109 Mekong ARCC

Climate Variability in South Asia

Satellite-derived environmental drivers for top predator hotspots

Lecture Prepared By: Mohammad Kamrul Arefin Lecturer, School of Business, North South University

Champaign-Urbana 2001 Annual Weather Summary

The Climate of Bryan County

The Climate of Marshall County

Yellow Sea Thermohaline and Acoustic Variability

Implementation of the Phoenix Visibility Monitoring Network

THE RESUSPENSION MODEL. Jan Macoun Czech Hydrometeorological Institute (CHMI), Prague, Czech Republic

8.1 Attachment 1: Ambient Weather Conditions at Jervoise Bay, Cockburn Sound

Funding provided by NOAA Sectoral Applications Research Project CLIMATE. Basic Climatology Colorado Climate Center

MAIN ATTRIBUTES OF THE PRECIPITATION PRODUCTS DEVELOPED BY THE HYDROLOGY SAF PROJECT RESULTS OF THE VALIDATION IN HUNGARY

The Climate of Grady County

Preliminary Conceptual Model Development

Changing Hydrology under a Changing Climate for a Coastal Plain Watershed

Applications of Meteorological Tower Data at Kennedy Space Center

Analysis of Historical Pattern of Rainfall in the Western Region of Bangladesh

Historical and Projected National and Regional Climate Trends

The Climate of Pontotoc County

HEATING THE ATMOSPHERE

IMPROVE MONITORING UPDATE VISIBILITY NEWS... Volume 1, No. 5 Fall 1992 January 1993

WIND DATA REPORT. Vinalhaven

Reactive Nitrogen Monitoring

A STUDY ON EVAPORATION IN IOANNINA, NW GREECE

Dust Storms of the Canadian Prairies: A Dustier and Muddier Outlook

Transcription:

Haze Communication using the CAMNET and IMPROVE Archives: Case Study at Acadia National Park Light absorption by fine Light scattering by fine Clear line of sight in absence of fine Light extinction is a function of the individual light absorption and light scattering properties of particles and gases present in the atmosphere. The figure above illustrates absorption and scattering of light by particles. With a clear line of sight, all of the incoming photons, as represented by the squiggly yellow lines, arrive unimpeded to the eye of the observer. Absorbing particles take up some of the incident photons, whereas scattering particles divert the path of photons. Total light extinction is frequently expressed as a light extinction coefficient (b ext ) in units of inverse length (such as Mm -1 ). In simple terms, the light extinction coefficient is a measure of the proportion of light lost per unit of distance traveled through the atmosphere. The light extinction coefficient, b ext, can be measured directly with a

transmissometer or determined empirically by reconstructing extinction as the sum of the scattering and absorption coefficients of the relevant particle constituents. The National Park Service s IMPROVE program developed the following representation for reconstructed extinction: b ext = b SO4 + b NO3 + b OrgC + b Soil + b Coarse + b ElemC + b Ray where the subscripts refer the aerosol component. (SO4 is sulfate, NO3 is nitrate, OrgC is organic carbon, soil is fine soil, coarse is coarse mass, elemc is elemental carbon and Ray is Rayleigh scattering. Note Rayleigh scattering, b Ray, is a measure of scattering due to air molecules. The Federal Land Managers Air Quality Related Values Workgroup (FLAG) uses a Rayleigh scattering value of 10 Mm -1 for the entire U.S. (FLAG, 2000). This value corresponds to Rayleigh conditions at about 1800 meters above sea level (Sisler and Malm, 2000). However, Rayleigh scattering varies with altitude and at sea level is estimated to be about 12 Mm -1 (Trijonis et al., 1990). It is understood that this reconstructed light extinction formula is not accurate for every sample, as it was designed to provide a consistent and replicable process for approximating light extinction based on observed relationships. The calculation of extinction coefficients for each individual chemical species can be described by the following equations (FLAG, 2000): b SO4 = 3[(NH 4 ) 2 SO 4 ]f(rh) b NO3 = 3[NH 4 NO 3 ]f(rh) b OrgC = 4[OrgC] b Soil = 1[Soil] b Coarse = 0.6[Coarse] b ElemC = 10[ElemC]. IMPROVE assumes that all sulfate is in the form ammonium sulfate ((NH 4 ) 2 SO 4 ) and that all nitrate is in the form ammonium nitrate (NH 4 NO 3 ). The bracketed quantities represent ambient air concentrations expressed in micrograms per cubic meter (µg/m 3 ). The numeric coefficients represent dry scattering efficiencies (m 2 /g), while the relative humidity adjustment factor f(rh) accounts for the hygroscopic properties of sulfate and nitrate (i.e. their tendency to absorb water in the atmosphere). As relative humidity increases this factor becomes larger, which in turn produces a higher coefficient of light extinction for the hygroscopic particles. Provided concentrations and humidity levels are known, the light extinction coefficients for individual particle constituents can be calculated and summed to estimate the overall light extinction coefficient, b ext. Keep in mind the above equations reflect simplified assumptions about the role of relative humidity and may not adequately account for the non-linear relationship between

humidity and particle growth rate. Under the Regional Haze regulations, monthly average values based on climatology are used for the relative humidity factor. To better represent visibility extinction based on daily PM averages, corresponding daily relative humidity values should be used. However, some uncertainty is introduced due to diurnal variations in both RH and PM constituent masses. Further uncertainty is introduced by assuming all sulfate particles are fully ammoniated, since this is not always the case; more acidic particles have a higher affinity for water uptake and would require a corresponding larger f(rh). Additionally, the above equations assume that organic carbon particles are nonhygroscopic and do not require a relative humidity adjustment. Whether or not a relative humidity adjustment factor should be applied to the organic fraction is an issue of current debate (Saxena et al., 1995) and is dependent upon the molecular makeup of the particles. Finally, the IMPROVE formulation was derived under the an assumption that the particles are externally mixed as opposed to the more likely case that each particle is a homogenous (internal) mixture of the individual components. This difference will affect the physical properties of the particle and in turn how they impact visibility. The sensitivity of reconstructed light extinction to each of these assumptions is an area that warrants further investigation. The CAMNET photo-archive has been developed to demonstrate the variations in visibility conditions that exist at Acadia. Using 24-hour average measured values of speciated particulate mass and relative humidity, the archive attempts to explain how variations in these measured quantities affect local visibility conditions. The photographs display current/representative visibility conditions at Acadia NP for worst, average and best days (High, Middle, Low days). The discussion assists the reader in investigating the interactions of relative humidity and fine mass on visibility and provides a means to compare the visibility impact of individual species. The first figure summarizes a range of visibility conditions for each of the four seasons. The next four pages of figures present the associated mass and visibility conditions. Discussions of these seasonal portraits are provided.

Text Descriptions for the Seasonal Figures: Spring: Three days were chosen based on the total aerosol extinction to represent the three regimes (Best, Middle, Worst) of visibility at Acadia during the spring. Analysis of the mass composition shows that the distribution among the various aerosol constituents are similar across visibility category, with the hygroscopic sulfate and nitrate components accounting for 62-70% of the fine mass. Organic and elemental carbon accounted for 18-26% of the mass. For these days, both mass and relative humidity differences contribute significantly to the predicted visibility differences. Mass differences between the worst and middle day account for the visibility differences, whereas differences in humidity account for the differences between the middle and best days. Based on the reconstructed extinction, clear differences should be discernible between all three cases. The worst day clearly shows the greatest impairment, while differences between the middle and best day are less obvious from the snapshots. Visibility degradation on the worst day is clearly dominated by higher mass values, with its humidity factor also playing a role. Differences between the middle and best summer day are predicted to be driven by differences in relative humidity. However, the 24-hour average f(rh) factor calculated for the middle day is substantially greater than the actual factor associated with the humidity levels depicted in the photograph since the early hours of the day experienced very high relatively humidity. The comparison of these two pictures illustrates the difficulty in combining 24-hour integrated or average measurements with instantaneous photographic results. Summer: Three days were chosen based on the total aerosol extinction to represent the three regimes (Best, Middle, Worst) of visibility at Acadia during the summer. Analysis of the mass composition shows that the distribution among the various aerosol constituents are somewhat varied across visibility category, with the hygroscopic sulfate and nitrate components accounting for 44-66% of the fine mass. Organic and elemental carbon accounted for 19-39% of the mass. For these days, both mass and relative humidity differences contribute significantly to the predicted visibility differences, with the relative humidity effects dominating. In fact, the mass loading of the middle day is less than that of the best, but the relative humidity factor is almost 3 times as large. Based on the reconstructed extinction, clear differences should be discernible between all three cases, and indeed, the worst day clearly shows the greatest impairment, followed by the middle day and then the best. The differences between the middle and best day is dominated by differences in f(rh), although the difference in mass also plays a role. Visibility degradation on the worst day is clearly dominated by high relative humidity, in addition to the relatively greater percentage of mass attributable to hygroscopic species ammonium sulfate and nitrate. Humidity levels on this day are sufficiently high that visibility could be diminished due to fog. Differences between the middle and best summer day are driven again primarily by differences in relative humidity and mass composition, with both higher humidity and hygroscopic mass on the middle day. These

effects outweigh the fact that 15% greater mass was measured on the best day, relative to the middle day. Fall: Three days were chosen based on the total aerosol extinction to represent the three regimes (Best, Middle, Worst) of visibility at Acadia during the fall. Analysis of the mass composition shows that the distribution among the various aerosol constituents are fairly similar across visibility category, with the hygroscopic sulfate and nitrate components accounting for 56-60% of the fine mass. Organic and elemental carbon accounted for 37-42% of the mass. For these days, both mass and relative humidity differences contribute significantly to the predicted visibility differences, with the higher mass values associated with greater visibility extinction. The relative humidity effect contributes over twice the punch to the middle day than it does to the best or worst day. Based on the reconstructed extinction, clear differences should be discernible between all three cases, and indeed, the worst day clearly shows the greatest impairment, followed by the middle day and then the best. The differences between the middle and best day is dominated by differences in f(rh), although the difference in mass also plays a role. Visibility degradation on the worst day is clearly dominated by the large observed particulate mass, more than 7 times the mass of the other days. This excessive particle loading more than outweighs the lower relative humidity effect on the worst day relative to the middle day. Winter: Three days were chosen based on the total aerosol extinction to represent the three regimes (Best, Middle, Worst) of visibility at Acadia during the winter. Analysis of the mass composition shows that the distribution among the various aerosol constituents are fairly similar across visibility category, with the hygroscopic sulfate and nitrate components accounting for 54-63% of the fine mass. Organic and elemental carbon accounted for 30-40% of the mass. For these days, both mass and relative humidity differences contribute significantly to the predicted visibility differences, with the higher mass and f(rh) values associated with greater visibility extinction. Based on the reconstructed extinction, clear differences should be discernible between all three cases. The worst day clearly shows greater impairment than do the other two days. The differences between the middle and best photos are subtle. The pictures capture one moment of the day, whereas the filter measurements and calculations of extinction are integrated over an entire 24-hour period. There is a factor of 2 difference in mass and 50% difference in associated f(rh). However, at the instance of the photographs, only a 10% difference in f(rh) was observed. Actual instantaneous mass differences are not available, but may be considerably less than the 24-hour averaged difference suggests. These observations highlight the difficulties in combining real-time photographs with time-integrated measurements.

20% Worst/Middle/Best Visibility at Acadia (April 2000 to September 2002) Winter Spring Summer Fall Jan 19 Mar 11 Jul 9 Nov 15 Jan 26 Apr 5 Aug 26 Oct 9 Jan 2 Mar 18 Aug 11 Nov 2

Spring Mar 11 10.8 µg/m 3 RH= 64% Apr 5 2.8 µg/m 3 RH= 57% PM 2.5 Mass Composition Visibility Extinction (Mm -1 ) 2% 3% 10% 15% 6% 3% 8% 6% 20% 64% 60% F(RH)= 4.0 B ext = 101 Mm -1 (NH4)2SO4 NH4NO3 OC EC Soil Coarse F(RH)= 4.1 B ext = 28 Mm -1 3% Mar 18 3.0 µg/m 3 RH= 27% 3% 14% 4% 17% 7% 55% F(RH)= 1.2 B ext = 11 Mm -1 0 15 30 45 60 75

Summer Mass Composition Visibility Extinction (Mm -1 ) Jul 9 5.8 µg/m 3 RH= 96% Aug 26 3.5 µg/m 3 RH= 57% 4% 7% 8% 7% 15% 1% 9% 13% 22% 9% 59% 46% F(RH)= 7.3 B ext = 93 Mm -1 (NH4)2SO4 NH4NO3 OC EC Soil Coarse F(RH)= 3.8 B ext = 29 Mm -1 Aug 11 4.0 µg/m 3 RH= 37% 5% 4% 12% 41% F(RH)= 1.3 B ext = 11 Mm -1 35% 3% 0 15 30 45 60 75

Fall Nov 15 15.7 µg/m 3 RH= 61% Oct 9 2.2 µg/m 3 RH= 87% Mass Composition Visibility Extinction (Mm -1 ) 5% 3% 32% 4% 9% 28% 13% 47% 53% F(RH)= 2.5 B ext = 101 Mm -1 (NH4)2SO4 NH4NO3 OC EC Soil Coarse F(RH)= 5.9 B ext = 29 Mm -1 6% Nov 2 1.6 µg/m 3 5% 2% RH= 67% 37% 50% F(RH)= 2.3 B ext = 11 Mm -1 6% 0 15 30 45

Winter Jan 19 7.1 µg/m 3 RH= 89% Jan 26 4.3 µg/m 3 RH= 55% Mass Composition Visibility Extinction (Mm -1 ) 8% 32% 6% 7% 24% 2% 12% 19% 46% 44% F(RH)= 5.0 B ext = 86 Mm -1 (NH4)2SO4 NH4NO3 OC EC Soil Coarse F(RH)= 2.3 B ext = 29 Mm -1 Jan 2 2.2 µg/m 3 RH= 51% 5% 27% 9% 5% 17% 37% F(RH)= 1.5 B ext = 11 Mm -1 0 15 30 45

30 "other" Soil 25 EC OMC 20 AmmNO3 AmmSO4 {S} 15 10 August 15, 2002 September 11, 2002 5 0 160 140 120 100 80 60 40 20 0 f(rh)=2.5 f(rh)=3.7 Bext Other Bext EC Bext OC Bext Hygro Two summertime days are compared. The visibility is quite poor for both days, based on the IMPROVE formula. Given the instantaneous photo versus the 24-hour average visibility calculation, this may not be the reality of the two pictures. Regardless, the main point to note here is that the particulate levels in the left figure are almost twice those in the right. However, due to higher humidity experienced on the day in the right side photo, the visibility is equally poor. This shows that even moderate pollution levels can lead to extremely poor visibility if the humidity is high and the level of hygroscopic particle constituents is appreciable.

12 10 8 "other" Soil EC OMC AmmNO3 AmmSO4 {S} g/m 3 6 July 30, 2001 4 July 13, 2002 2 0 Bext 50 45 40 35 30 25 20 15 Other Bext EC Bext OC Bext Hygro 10 5 0 f(rh)=1.80 [1.2 for 9-5] f(rh)=1.76 [1.5 for 9-5] Two summertime days are compared. The visibility is moderate for both days, based on the IMPROVE formula. Given the instantaneous photo versus the 24-hour average visibility calculation, the true extinction may be different. Here, visibility is slightly worse in the right-hand photograph. Based on the measured values, this is likely due to higher organic carbon levels measured on that day. The contribution due to hygroscopics is similar on both days. Note that the f(rh) values are similar when averaged over the 24-hour period, but in reality are slightly higher for the right-hand picture at the time of the photos. Since the hourly f(rh) is lower than the daily average (which is used in the bar charts), the bar chart may overestimate the relative contribution of the hygroscopics. Since we do not know how the actual levels of OC and sulfate at the time of the photo, the true visibility contributions cannot be determined.

The main idea in the final two pictoral presentations is to show that humidity levels, particle levels, and particle constituents all play a role in determining the visibility conditions. This effort also demonstrated the drawback of comparing 24-hour particle and humidity measurements with instantaneous photographs. With the new RAIN network collection hourly measurements of sulfate and bi-hourly levels of carbon, a more fruitful comparison with the CAMNET photos can be conducted. This may prove highly valuable in clarifying the roles of humidity and fine particle make-up on visibility conditions.